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Determining the Speed of Light

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Determining the Speed of Light ! Determining the Speed of Light The speed of light is one of the most important constants in physical science. In addition to the basic role it plays in the theory of relativity, its value is required for work in photonics, electronics, electromagnetism, quantum theory and nuclear physics. For this reason, a great deal of time and energy has been devoted to its determination. Although its measurement has occupied many scientists from the time of Galileo to the present day, it was the work of British physicist, Louis Essen, that led to the present accepted value and the subsequent re-definition of the unit of length (metre) in terms of the speed of light. Louis Essen is better known for building the first operational atomic clock in 1955 but he was also aware that there was an urgent need for better long-range radio- navigation aids at the end of the Second World War; and knowing the exact value of the speed of light was as important as precise time measurement for determining the location of an aircraft, ship or submarine. Essen worked at the National Physical Laboratory, Teddington, UK (NPL) during the war and his experience with radar and microwave devices, especially the cavity resonator, enabled him to develop a non-optical method of measuring the speed of light. In 1946, he published a new value of the speed of light in vacuum (299,792 ± 3 km/ s) that was 16 km/s higher than the then accepted value. His findings caused a great deal of controversy at the time and were not accepted for several years. I have reproduced a part of my father-in-law’s memoirs below in which he describes how he came to be involved in measuring the speed of light. Ray Essen Memoirs of Louis Essen The exact value of the speed of light was needed during the Second World War for microwave applications such as radar and aircraft radio-navigation systems. NPL (Britain’s national measurement institute) occasionally received enquiries from people working on radar who were concerned about the best value to use and the telephone operators usually directed the callers to me. At first, I gave the textbook value of 299,800 km/s or, if a higher accuracy seemed appropriate, 299,776 ± 4 km/s, which was the value that Raymond Birge at the University of California in Berkeley had derived in 1941 from a statistical appraisal of earlier optical determinations. These enquiries set me thinking about the speed of light and how accurately it was actually known. My work with cavity wavemeters led me to believe that I could measure its value with a higher accuracy than could be determined by optical methods. Albert A Michelson The accepted value for the speed of light before the Second World War was based largely on the results of Michelson and his co-workers in the USA, and particularly on his last experiment made in 1935. This was performed with the encouragement and support of international bodies; it was costly and widely publicised. One feature which made it costly, and was thought to be in its favour, was that the light path was confined in an evacuated pipe 1.6-km long to eliminate the effect of the refractive index of the air which reduces the speed by about 0.03 percent. Previous measurements had all been made in air and corrected for refractive index, which was calculated from the atmospheric conditions at the time. The reviewers’ faith in the result was strengthened by the fact that four subsequent determinations made by different scientists in different countries were in close agreement with it. A study of the original papers convinced me that the value was not nearly so well established as was thought. The actual precision of measurement was low and the results were an average of many, sometimes thousands, of individual measurements, always an unsatisfactory procedure. The authors of these papers made no great claims for the accuracy of their results and pointed out that unexplained discrepancies were present. Cavity Resonator Method My experience made me confident that the speed of light could be obtained far more accurately as well as far more simply by measuring the dimensions and resonant frequency of a specially constructed microwave cavity wavemeter. The setting to resonance is so precise that a single measurement would be more accurate than the average of the large numbers taken in the optical determinations and the high precision would make it possible to investigate and eliminate the effect of small systematic errors. In view of its importance in radio navigation I started a more systematic study of the speed of light as a side-line to my normal duties. At the end of the Second World War, NPL already had a full programme of work intended to assist in the recovery of Britain’s industry and a new determination of the speed of light was not considered to be of high priority. Consequently, I was initially obliged to undertake this work in my spare time and no objections were raised. I devised an experimental method that enabled me to assemble most of the necessary apparatus from old pieces of war- surplus equipment. A visitor from the USA mentioned that William Webster (‘Bill’) Hansen at Stanford University was contemplating a similar measurement. But it is no bad thing to duplicate work of this kind and, although Hansen was one of the pioneers of cavity resonator theory, NPL was better equipped on the technical side. We had then the best frequency standards and microwave measuring experience in the world, a splendid workshop where the resonator could be made and a metrology department where its dimensions could be measured. All these facilities were situated in the same grounds and collaboration between the staff was encouraged. This last point proved to be most important. There was a slight discrepancy between some of the metrological measurements which were discussed with the head of the department. In the course of the discussions it occurred to him that there might also be a systematic error. The internal diameter had been measured by their standard method in which two small balls at the ends of the arms of a feeler gauge slide over the curved surface. The pressure of the balls on the surface causes a slight depression that must be corrected for, and as the gauges usually tested are all made from steel a standard correction is included in the calculations. But our resonator was made of copper, a softer metal, and a larger correction should be applied. His suspicions were correct and a small but significant error was avoided through the close relationship between our departments. The frequency measurements were made with the help of Albert Gordon-Smith, a skilled and meticulously careful experimenter. Our result, published in 1946, was 16 km/s higher than the accepted value, which was much more interesting than if it had been confirmed. It did not surprise us but everyone else was very sceptical, even our Director, who, while congratulating us on the work, suggested that we would no doubt get the correct result when we had perfected the technique. The radar establishments in the UK and the USA, who were the people most concerned, continued to use the old value for several years showing that scientists can get fixed ideas on poor evidence and refused to relinquish them. No result had been published from Stanford but a report in a popular journal suggested that the result was going to confirm the optical value. I was planning a visit to the USA at that time so our Director suggested that I should go and see them. Unfortunately, I found that Hansen was in hospital with pneumonia which proved fatal. His colleagues were not in a position to give a value but later when it was published in a short note it was quite near to the NPL result, being 3 km/s lower. Revised Method of Measurement There was now a post-war reshuffle of staff and I moved back to the Electricity Division where, in 1950, I was able to repeat the speed-of-light measurement with a different form of resonator. The weakest point of the first experiment seemed to be the measurement of the dimensions. Apart from the metrological difficulty, it was known that the electric and magnetic fields penetrated the surfaces of the cavity resonator which increased the effective size of the metal cylinder. The penetration is zero for perfect conductors but it is not negligible for copper (used in the first experiment) despite it being one of the best conductors we have. I calculated the correction factor from transmission-line theory but the computer genius, Alan Turing who was then working at NPL, repeated the calculation elegantly and rigorously for me from waveguide theory. I found later that it had been calculated and published in a French journal. In any case, I managed to eliminate most of the correction by a suitable design of cavity resonator. The length could be altered by a piston and the wavelength found by the distance between two successive resonances, thus eliminating the effect of penetration in the end faces. Then, by using a number of different frequencies and different modes of resonance, it was possible to eliminate the diameter from the calculations or, expressed differently, to measure the diameter in terms of length and frequency. It was clearly a more complicated and difficult experiment than before and I was fortunate in securing the help of our excellent workshops and of Eric Hope, another skilled electronic expert to replace Gordon- Smith, whom I had lost in the move.
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